P
US8403549B2ActiveUtilityPatentIndex 38

Optical device with lenticular arrays, edge-type backlight module and direct-type backlight module

Assignee: Lin hao xiangPriority: Jul 1, 2010Filed: Nov 11, 2010Granted: Mar 26, 2013
Est. expiryJul 1, 2030(~4 yrs left)· nominal 20-yr term from priority
Inventors:LIN HAO-XIANGCHEN YAN-ZUOCHENG WEN-FENGCHANG JUI-HSIANG
G02B 3/0056G02F 1/133607G02F 1/133606G02B 3/005G02B 6/005
38
PatentIndex Score
0
Cited by
5
References
10
Claims

Abstract

An edge-type backlight module and a direct-type backlight module with a optical device are provided. The optical device comprises an array layer and a second refractive layer. The array layer has a first refractive index (n 1 ) and contains pluralities of lenticular lens disposed on a base surface side by side. The lenticular lens contains a curving structure with a peak, a trough, a curvature radius (R), a width (P) and an altitude (H) between the peak and the trough. The trough is disposed on the base1 surface. The array layer has a first critical angle (θ 1c ) relative to the normal of the base surface and satisfies θ 1 ⁢ c = sin - 1 ⁡ ( 1 n 1 ) and H = R 1 + K ⁡ [ 1 - 1 - ( 1 + K ) ⁢ ( P 2 ⁢ R ) 2 ] . The conical constant (K) of the lenticular lens ranges from −2.1 to −1.5. The second refractive layer is adjacent to the array layer and has a second refractive index (n 2 ) and a second critical angle (θ 2c ) relative to the normal line of the second refractive layer. The first refractive index (n 1 ) is greater than the second refractive index (n 2 ) and θ 2 ⁢ c = sin - 1 ⁡ ( n 2 n 1 ) is satisfied. Wherein the lenticular lens, the first critical angle (θ 1c ) and the second critical angle (θ 2c ) satisfy the equation of sin - 1 ⁡ ( 1 n 1 ) ≤ cot - 1 ⁡ ( H P / 2 ) < sin - 1 ⁡ ( n 2 n 1 ) .

Claims

exact text as granted — not AI-modified
We claim: 
     
       1. An optical device with lenticular arrays, comprising:
 an array layer having a first refractive index (n 1 ) and comprising pluralities of lenticular lenses disposed on a base surface side by side, each of the lenticular lenses containing a curving structure with a peak, a trough, a curvature radius (R), a width (P) and an altitude (H) between the peak and the trough, the trough being disposed on the base surface, the array layer having a first critical angle (θ 1c ) relative to the normal line of the base surface and satisfying 
 
       
         
           
             
               
                 θ 
                 
                   1 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   c 
                 
               
               = 
               
                 
                   sin 
                   
                     - 
                     1 
                   
                 
                 ⁡ 
                 
                   ( 
                   
                     1 
                     
                       n 
                       1 
                     
                   
                   ) 
                 
               
             
           
         
       
       and 
       
         
           
             
               
                 H 
                 = 
                 
                   
                     R 
                     
                       1 
                       + 
                       K 
                     
                   
                   ⁡ 
                   
                     [ 
                     
                       1 
                       - 
                       
                         
                           1 
                           - 
                           
                             
                               ( 
                               
                                 1 
                                 + 
                                 K 
                               
                               ) 
                             
                             ⁢ 
                             
                               
                                 ( 
                                 
                                   P 
                                   
                                     2 
                                     ⁢ 
                                     R 
                                   
                                 
                                 ) 
                               
                               2 
                             
                           
                         
                       
                     
                     ] 
                   
                 
               
               , 
             
           
         
       
       the conical constant (K) of the lenticular lens ranging from −2.1 to −1.5;
 a second refractive layer being adjacent to the array layer and having a second refractive index (n 2 ) and a second critical angle (θ 2c ) relative to the normal line of the second refractive layer, the first refractive index (n 1 ) being greater than the second refractive index (n 2 ) and 
 
       
         
           
             
               
                 θ 
                 
                   2 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   c 
                 
               
               = 
               
                 
                   sin 
                   
                     - 
                     1 
                   
                 
                 ⁡ 
                 
                   ( 
                   
                     
                       n 
                       2 
                     
                     
                       n 
                       1 
                     
                   
                   ) 
                 
               
             
           
         
       
       being satisfied;
 wherein the lenticular lens, the first critical angle (θ 1c ) and the second critical angle (θ 2c ) satisfy the equation of 
 
       
         
           
             
               
                 
                   sin 
                   
                     - 
                     1 
                   
                 
                 ⁡ 
                 
                   ( 
                   
                     1 
                     
                       n 
                       1 
                     
                   
                   ) 
                 
               
               ≤ 
               
                 
                   cot 
                   
                     - 
                     1 
                   
                 
                 ⁡ 
                 
                   ( 
                   
                     H 
                     
                       P 
                       ⁢ 
                       
                         / 
                       
                       ⁢ 
                       2 
                     
                   
                   ) 
                 
               
               < 
               
                 
                   
                     sin 
                     
                       - 
                       1 
                     
                   
                   ⁡ 
                   
                     ( 
                     
                       
                         n 
                         2 
                       
                       
                         n 
                         1 
                       
                     
                     ) 
                   
                 
                 . 
               
             
           
         
       
     
     
       2. The optical device with lenticular arrays as  claim 1 , wherein a first thickness (t 1 ) ranges from the base surface to the interface between the array layer and the second refractive layer, and the second refractive layer has a second thickness (t 2 ), in which the value of t 2 /t 1  ranges from 0.035 to 0.084. 
     
     
       3. The optical device with lenticular arrays as  claim 1 , wherein the conical constant (K) of the lenticular lens ranges from −2 to −1.65. 
     
     
       4. The optical device with lenticular arrays as  claim 1 , wherein the value of H/P ranges from 0.42 to 0.498. 
     
     
       5. The optical device with lenticular arrays as  claim 1 , wherein the array layer is expanded to 2-Dimension. 
     
     
       6. The optical device with lenticular arrays as  claim 1 , wherein the array layer is expanded to 3-Dimension. 
     
     
       7. The optical device with lenticular arrays as  claim 1 , wherein the optical device further comprises a third refractive layer with a third refractive index (n 3 ), in which n 3  is smaller than n 1  and n 2 . 
     
     
       8. The optical device with lenticular arrays as  claim 1 , wherein the material of the array layer or the second refractive layer is polyethylene terephthalate (PET), polycarbonate (PC), tri-acetyl cellulose (TAC), polymethylmethacrylate (PMMA), methylmethacrylate styrene, polystyrene (PS) or cyclic olefin copolymer (COC). 
     
     
       9. An edge-type backlight module for transmitting an incident light, a first optical path and a second optical path, comprising:
 a light source for emitting the incident light; 
 a light guide plate disposed at one side of the light source and receiving the incident light and transmitting the optical path; 
 a reflective plate disposed at beneath of the light guide plate; 
 an optical device with lenticular arrays disposed above the light guide plate to receive optical path, and having an array layer containing a first refractive index (n 1 ) and comprising pluralities of lenticular lenses disposed on a base surface side by side, each of the lenticular lenses containing a curving structure with a peak, a trough, a curvature radius (R), a width (P) and an altitude (H) between the peak and the trough, the trough being disposed on the base surface, the array layer having a first critical angle (θ 1c ) relative to the normal line of the base surface and satisfying 
 
       
         
           
             
               
                 θ 
                 
                   1 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   c 
                 
               
               = 
               
                 
                   sin 
                   
                     - 
                     1 
                   
                 
                 ⁡ 
                 
                   ( 
                   
                     1 
                     
                       n 
                       1 
                     
                   
                   ) 
                 
               
             
           
         
       
       and 
       
         
           
             
               
                 H 
                 = 
                 
                   
                     R 
                     
                       1 
                       + 
                       K 
                     
                   
                   ⁡ 
                   
                     [ 
                     
                       1 
                       - 
                       
                         
                           1 
                           - 
                           
                             
                               ( 
                               
                                 1 
                                 + 
                                 K 
                               
                               ) 
                             
                             ⁢ 
                             
                               
                                 ( 
                                 
                                   P 
                                   
                                     2 
                                     ⁢ 
                                     R 
                                   
                                 
                                 ) 
                               
                               2 
                             
                           
                         
                       
                     
                     ] 
                   
                 
               
               , 
             
           
         
       
       the conical constant (K) of the lenticular lens ranging from −2.1 to −1.5;
 a second refractive layer being adjacent to the array layer and having a second refractive index (n 2 ) and a second critical angle (θ 2c ) relative to the normal line of the second refractive layer, the first refractive index (n 1 ) being greater than the second refractive index (n 2 ) and 
 
       
         
           
             
               
                 θ 
                 
                   2 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   c 
                 
               
               = 
               
                 
                   sin 
                   
                     - 
                     1 
                   
                 
                 ⁡ 
                 
                   ( 
                   
                     
                       n 
                       2 
                     
                     
                       n 
                       1 
                     
                   
                   ) 
                 
               
             
           
         
       
       being satisfied;
 wherein the lenticular lens, the first critical angle (θ 1c ) and the second critical angle (θ 2c ) satisfy the equation of 
 
       
         
           
             
               
                 
                   
                     sin 
                     
                       - 
                       1 
                     
                   
                   ⁡ 
                   
                     ( 
                     
                       1 
                       
                         n 
                         1 
                       
                     
                     ) 
                   
                 
                 ≤ 
                 
                   
                     cot 
                     
                       - 
                       1 
                     
                   
                   ⁡ 
                   
                     ( 
                     
                       H 
                       
                         P 
                         ⁢ 
                         
                           / 
                         
                         ⁢ 
                         2 
                       
                     
                     ) 
                   
                 
                 < 
                 
                   
                     sin 
                     
                       - 
                       1 
                     
                   
                   ⁡ 
                   
                     ( 
                     
                       
                         n 
                         2 
                       
                       
                         n 
                         1 
                       
                     
                     ) 
                   
                 
               
               , 
             
           
         
       
       and the first optical path is modified by means of the first critical angle (θ 1c ) and the second critical angle (θ 2c ) so that the second optical path and total reflection to the reflective plate are generated. 
     
     
       10. A direct-type backlight module for transmitting a incident light, a first optical path and a second optical path, comprising:
 a light source for emitting the incident light; 
 a reflective plate disposed at beneath of the light source; 
 a diffusive plate disposed above the light source and receiving the incident light and transmitting the optical path; 
 an optical device with lenticular arrays disposing above the diffusive plate to receive optical path, and having an array layer containing a first refractive index (n 1 ) and comprising pluralities of lenticular lenses disposed on a base surface side by side, each of the lenticular lenses containing a curving structure with a peak, a trough, a curvature radius (R), a width (P) and an altitude (H) between the peak and the trough, the trough being disposed on the base surface, the array layer having a first critical angle (θ 1c ) relative to the normal line of the base surface and satisfying 
 
       
         
           
             
               
                 θ 
                 
                   1 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   c 
                 
               
               = 
               
                 
                   sin 
                   
                     - 
                     1 
                   
                 
                 ⁡ 
                 
                   ( 
                   
                     1 
                     
                       n 
                       1 
                     
                   
                   ) 
                 
               
             
           
         
       
       and 
       
         
           
             
               
                 H 
                 = 
                 
                   
                     R 
                     
                       1 
                       + 
                       K 
                     
                   
                   ⁡ 
                   
                     [ 
                     
                       1 
                       - 
                       
                         
                           1 
                           - 
                           
                             
                               ( 
                               
                                 1 
                                 + 
                                 K 
                               
                               ) 
                             
                             ⁢ 
                             
                               
                                 ( 
                                 
                                   P 
                                   
                                     2 
                                     ⁢ 
                                     R 
                                   
                                 
                                 ) 
                               
                               2 
                             
                           
                         
                       
                     
                     ] 
                   
                 
               
               , 
             
           
         
       
       the conical constant (K) of the lenticular lens ranging from −2.1 to −1.5;
 a second refractive layer being adjacent to the array layer and having a second refractive index (n 2 ) and a second critical angle (θ 2c ) relative to the normal line of the second refractive layer, the first refractive index (n 1 ) being greater than the second refractive index (n 2 ) and 
 
       
         
           
             
               
                 θ 
                 
                   2 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   c 
                 
               
               = 
               
                 
                   sin 
                   
                     - 
                     1 
                   
                 
                 ⁡ 
                 
                   ( 
                   
                     
                       n 
                       2 
                     
                     
                       n 
                       1 
                     
                   
                   ) 
                 
               
             
           
         
       
       being satisfied;
 wherein the lenticular lens, the first critical angle (θ 1c ) and the second critical angle (θ 2c ) satisfy the equation of 
 
       
         
           
             
               
                 
                   
                     sin 
                     
                       - 
                       1 
                     
                   
                   ⁡ 
                   
                     ( 
                     
                       1 
                       
                         n 
                         1 
                       
                     
                     ) 
                   
                 
                 ≤ 
                 
                   
                     cot 
                     
                       - 
                       1 
                     
                   
                   ⁡ 
                   
                     ( 
                     
                       H 
                       
                         P 
                         ⁢ 
                         
                           / 
                         
                         ⁢ 
                         2 
                       
                     
                     ) 
                   
                 
                 < 
                 
                   
                     sin 
                     
                       - 
                       1 
                     
                   
                   ⁡ 
                   
                     ( 
                     
                       
                         n 
                         2 
                       
                       
                         n 
                         1 
                       
                     
                     ) 
                   
                 
               
               , 
             
           
         
       
       and the first optical path is modified by means of the first critical angle (θ 1c ) and the second critical angle (θ 2c ) so that the second optical path and total reflection to the reflective plate are generated.

Cited by (0)

No later patents cite this yet.

References (0)

No backward citations on record.